CA2839763C - Electromagnetically heated thermal flowmeter for wellbore fluids - Google Patents
Electromagnetically heated thermal flowmeter for wellbore fluids Download PDFInfo
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- CA2839763C CA2839763C CA2839763A CA2839763A CA2839763C CA 2839763 C CA2839763 C CA 2839763C CA 2839763 A CA2839763 A CA 2839763A CA 2839763 A CA2839763 A CA 2839763A CA 2839763 C CA2839763 C CA 2839763C
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- 239000012530 fluid Substances 0.000 title claims abstract description 100
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims abstract description 31
- 238000000034 method Methods 0.000 claims abstract description 28
- 239000000523 sample Substances 0.000 claims abstract description 25
- 238000010438 heat treatment Methods 0.000 claims abstract description 24
- 238000004519 manufacturing process Methods 0.000 claims description 9
- 239000004215 Carbon black (E152) Substances 0.000 claims description 6
- 229930195733 hydrocarbon Natural products 0.000 claims description 6
- 150000002430 hydrocarbons Chemical class 0.000 claims description 6
- 230000001678 irradiating effect Effects 0.000 claims description 4
- 239000000203 mixture Substances 0.000 abstract 1
- 239000003921 oil Substances 0.000 description 25
- 230000005855 radiation Effects 0.000 description 12
- 239000000470 constituent Substances 0.000 description 6
- 238000010521 absorption reaction Methods 0.000 description 4
- 238000012544 monitoring process Methods 0.000 description 4
- 230000005540 biological transmission Effects 0.000 description 3
- 230000000875 corresponding effect Effects 0.000 description 3
- 239000008236 heating water Substances 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- 230000015572 biosynthetic process Effects 0.000 description 2
- 238000004891 communication Methods 0.000 description 2
- 230000002596 correlated effect Effects 0.000 description 2
- 239000011159 matrix material Substances 0.000 description 2
- 238000011144 upstream manufacturing Methods 0.000 description 2
- 239000004593 Epoxy Substances 0.000 description 1
- -1 Kevlar0 Substances 0.000 description 1
- 239000012223 aqueous fraction Substances 0.000 description 1
- 239000004760 aramid Substances 0.000 description 1
- 229920003235 aromatic polyamide Polymers 0.000 description 1
- 238000009529 body temperature measurement Methods 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 229920001577 copolymer Polymers 0.000 description 1
- 239000010779 crude oil Substances 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
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- 239000003822 epoxy resin Substances 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
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Classifications
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/68—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using thermal effects
- G01F1/684—Structural arrangements; Mounting of elements, e.g. in relation to fluid flow
- G01F1/688—Structural arrangements; Mounting of elements, e.g. in relation to fluid flow using a particular type of heating, cooling or sensing element
-
- E—FIXED CONSTRUCTIONS
- E21—EARTH OR ROCK DRILLING; MINING
- E21B—EARTH OR ROCK DRILLING; OBTAINING OIL, GAS, WATER, SOLUBLE OR MELTABLE MATERIALS OR A SLURRY OF MINERALS FROM WELLS
- E21B47/00—Survey of boreholes or wells
- E21B47/10—Locating fluid leaks, intrusions or movements
- E21B47/103—Locating fluid leaks, intrusions or movements using thermal measurements
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/704—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow using marked regions or existing inhomogeneities within the fluid stream, e.g. statistically occurring variations in a fluid parameter
- G01F1/7044—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow using marked regions or existing inhomogeneities within the fluid stream, e.g. statistically occurring variations in a fluid parameter using thermal tracers
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/704—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow using marked regions or existing inhomogeneities within the fluid stream, e.g. statistically occurring variations in a fluid parameter
- G01F1/708—Measuring the time taken to traverse a fixed distance
- G01F1/7084—Measuring the time taken to traverse a fixed distance using thermal detecting arrangements
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/68—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using thermal effects
- G01F1/684—Structural arrangements; Mounting of elements, e.g. in relation to fluid flow
- G01F1/688—Structural arrangements; Mounting of elements, e.g. in relation to fluid flow using a particular type of heating, cooling or sensing element
- G01F1/6888—Thermoelectric elements, e.g. thermocouples, thermopiles
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- Physics & Mathematics (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- Life Sciences & Earth Sciences (AREA)
- Engineering & Computer Science (AREA)
- Geology (AREA)
- Mining & Mineral Resources (AREA)
- Geophysics (AREA)
- Environmental & Geological Engineering (AREA)
- General Life Sciences & Earth Sciences (AREA)
- Geochemistry & Mineralogy (AREA)
- Measuring Volume Flow (AREA)
Abstract
A method of measuring multiphase flow of components in a wellbore fluid mixture by selectively heating components (e.g. oil and water) in the flow with electromagnetic energy, and detecting the heated components at a known distance downstream. The flow and velocity of components in the flow stream can be estimated with the present method. Example types of electromagnetic waves include infrared, microwaves, and radio waves. The different components can be heated simultaneously or at different times. The heated components can be detected with one or more temperature probes, and oil wet or water wet probes can be used to improve thermal contact to the corresponding components in the fluid stream.
Description
ELECTROMAGNETICALLY HEATED THERMAL FLOWMETER FOR
WELLBORE FLUIDS
BACKGROUND
1. Field of Invention [0001] The invention relates generally to a flowmeter for measuring multiphase flow of wellbore fluids in a tubular. More specifically, the present invention relates to a flowmeter that heats a particular constituent in the flow stream electromagnetically and then measures the time delay until a temperature response is detected at some known distance downstream of the heating so as to estimate a flow velocity of that constituent.
WELLBORE FLUIDS
BACKGROUND
1. Field of Invention [0001] The invention relates generally to a flowmeter for measuring multiphase flow of wellbore fluids in a tubular. More specifically, the present invention relates to a flowmeter that heats a particular constituent in the flow stream electromagnetically and then measures the time delay until a temperature response is detected at some known distance downstream of the heating so as to estimate a flow velocity of that constituent.
2. Description of Prior Art [0002] Flowmeters are often used for measuring flow of fluid produced from hydrocarbon producing wellbores. Flowmeters may be deployed downhole within a producing wellbore, a jumper or caisson used in conjunction with a subsea wellbore, or a production transmission line used in distributing the produced fluids. Monitoring fluid produced from a wellbore is useful in wellbore evaluation and to project production life of a well. In some instances transmission lines may include fluid produced from wells having different owners. Therefore proper accounting requires a flow measuring device that monitors the flow contribution from each owner.
[0003] The produced fluid may include water and/or gas mixed with liquid hydrocarbon.
Knowing the water fraction is desirable to ensure adequate means are available for separating the water from the produced fluid. Additionally, the amount and presence of gas is another indicator of wellbore performance, and vapor mass flow impacts transmission requirements. Flowmeters can be employed that provide information regarding total flow, water cut amount, and gas fractions. However, these often require periodic analysis of the fluid entering the flowmeter.
This may involve deploying a sample probe upstream of the flowmeter; which can produce inaccuracy, and may interrupt or temporarily halt fluid production.
SUMMARY OF THE INVENTION
Knowing the water fraction is desirable to ensure adequate means are available for separating the water from the produced fluid. Additionally, the amount and presence of gas is another indicator of wellbore performance, and vapor mass flow impacts transmission requirements. Flowmeters can be employed that provide information regarding total flow, water cut amount, and gas fractions. However, these often require periodic analysis of the fluid entering the flowmeter.
This may involve deploying a sample probe upstream of the flowmeter; which can produce inaccuracy, and may interrupt or temporarily halt fluid production.
SUMMARY OF THE INVENTION
[0004] The present disclosure includes a method and apparatus for measuring a flow of wellbore fluid by heating a fluid constituent with a wave of electromagnetic energy, and then detecting when the heated fluid reaches a location downstream at a known distance from where the fluid was heated. In an example embodiment, a method of measuring flow of a component of a wellbore fluid stream is disclosed that includes heating the component with an electromagnetic wave of a wavelength that the component absorbs. The temperature of the fluid stream downstream of where the fluid stream is being irradiated is monitored to detect when the temperature of the fluid stream increases due to heating with the electromagnetic wave. The velocity of the component is estimated based on the distance between where the fluid stream is being irradiated and where the temperature is being measured, and the time between when the fluid is heated and when the fluid stream temperature increases. In an example, the component is a first component and the fluid stream includes a second component, the second component is heated by irradiating the fluid stream with an electromagnetic wave having a wavelength that is absorbed by the second component. The velocity of the second component is estimated in a same way as for the first component. In an example embodiment, the first component can be a hydrocarbon. In an alternative, the wavelength of the electromagnetic wave can be about 1740 nanometers, which is a near infrared absorption peak for oil. Optionally, the frequency of the electromagnetic wave can have a value of about 15 MHz or about 5 MHz, which are microwave regions where crude oils preferentially absorb. In an example embodiment, the first component comprises water. In an alternative, the wavelength of the electromagnetic wave is about 1450 nanometers, which is a near infrared absorption peak for water. Optionally, the wavelength of the electromagnetic wave is about 1930 nanometers, which is another near infrared absorption peak for water. In an example, the frequency of the electromagnetic wave is about 18 GHz, which is a microwave region at which water preferentially absorbs. Other electromagnetic wavelengths at which the absorption of water and oil are very different may also be used.
[0005] Also disclosed herein is a method of measuring a flow of a wellbore fluid that in an example embodiment includes heating oil in the flow of wellbore fluid by directing infrared radiation into the flow, detecting a temperature change in the fluid downstream of where the infrared radiation is directed into the flow that is caused by the infrared radiation heating the oil, estimating a velocity of the oil in the flow that is based on a time difference between when the oil is heated by the infrared radiation and when the temperature change in the fluid is sensed that is caused by the infrared radiation heating the oil. The method further includes heating water in the flow of wellbore fluid by directing infrared radiation into the flow, detecting a temperature change in the fluid downstream of where the infrared radiation is directed into the flow that is caused by the infrared radiation heating the water, and estimating a velocity of the water in the flow that is based on a time difference between when the water is heated by the infrared radiation and when the temperature change in the fluid is sensed that is caused by the infrared radiation heating the water. In an example embodiment of the method, the infrared radiation for heating the oil has a wavelength of around 1740 nanometers. In an example embodiment of the method, the infrared radiation for heating the water, the wavelength is about 1450 nanometers or about 1930 nanometers.
[0006] In another example method, flow of one or more fluid components flowing in a stream of a wellbore fluid is evaluated. In an example embodiment of this method the stream of wellbore fluid is irradiated by a microwave with a frequency that is absorbed by the fluid component thereby heating the fluid component, a temperature of the stream of wellbore fluid is monitored at a location downstream of where the microwave is directed into the stream, a change in temperature of the stream of wellbore fluid is detected downstream of where the microwave is directed into the stream that is caused by directing the microwave into the stream of wellbore fluid. A velocity of the component is estimated based on a time difference between when the microwave is directed into the stream and when the change in temperature is detected, and a distance difference between where the microwave is directed into the stream and where the change in temperature is detected. Optionally, the component is oil. In an example when the component is oil, the frequency of the microwave can be about 5 MHz or about 15 MHz. In an alternate embodiment the component is water. In an example when the component is water the frequency of the microwave is about 18 GHz. In an example embodiment, the fluid includes oil and water components, and microwaves are directed into the fluid to heat both water and oil, and oil wet temperature probe and a water wet temperature probes, which should have better thermal contact with their corresponding components, are disposed downstream for monitoring temperature changes. Thus the oil and water components can be heated at substantially the same time and the heating of the oil and water components can be detected at substantially the same time.
[0006a] Also disclosed herein a method of measuring flow of a component of an oil and gas wellbore fluid stream, the method comprising: a. installing a flowmeter in a production tube of the wellbore, the flowmeter comprising a transmitter device capable of transmitting at least two electromagnetic waves with different frequencies and a temperature sensor; b.
selecting an electromagnetic wave having a predetermined wavelength that is absorbed by a component that is expected to be present in the fluid stream; c. heating the component by irradiating with the transmitter device the fluid stream with the electromagnetic wave having the wavelength that is absorbed by the component expected to be present in the fluid stream;
d. sensing with the temperature sensor a temperature of the fluid stream downstream of where the fluid stream is being irradiated; e. detecting when the temperature of the fluid stream downstream of where the fluid stream is being irradiated increases due to heating with the electromagnetic wave; and f. estimating a velocity of the component expected to be present in the flow based on a distance between where the fluid stream is being irradiated and where the temperature of the fluid stream is being sensed and a time of heating of step (c) and a time of detecting of step (e).
-4a-, , BRIEF DESCRIPTION OF DRAWINGS
[0006a] Also disclosed herein a method of measuring flow of a component of an oil and gas wellbore fluid stream, the method comprising: a. installing a flowmeter in a production tube of the wellbore, the flowmeter comprising a transmitter device capable of transmitting at least two electromagnetic waves with different frequencies and a temperature sensor; b.
selecting an electromagnetic wave having a predetermined wavelength that is absorbed by a component that is expected to be present in the fluid stream; c. heating the component by irradiating with the transmitter device the fluid stream with the electromagnetic wave having the wavelength that is absorbed by the component expected to be present in the fluid stream;
d. sensing with the temperature sensor a temperature of the fluid stream downstream of where the fluid stream is being irradiated; e. detecting when the temperature of the fluid stream downstream of where the fluid stream is being irradiated increases due to heating with the electromagnetic wave; and f. estimating a velocity of the component expected to be present in the flow based on a distance between where the fluid stream is being irradiated and where the temperature of the fluid stream is being sensed and a time of heating of step (c) and a time of detecting of step (e).
-4a-, , BRIEF DESCRIPTION OF DRAWINGS
[0007]
Some of the features and benefits of the present invention having been stated, others will become apparent as the description proceeds when taken in conjunction with the accompanying drawings, in which:
Some of the features and benefits of the present invention having been stated, others will become apparent as the description proceeds when taken in conjunction with the accompanying drawings, in which:
[0008] FIG. 1 is a side perspective view of an example embodiment of a flowmeter coupled with a tubular in accordance with the present invention.
[0009] FIG. 2 is a side partial sectional view of an embodiment of the flowmeter of FIG. 1 disposed in production tubing.
[0010] FIGS. 3-6 are side sectional views of embodiments of the flowmeter of FIG. 1 at operational sequences.
[0011] FIG. 7 is a side partial sectional view of an embodiment of the flowmeter of FIG. 1 disposed in a downhole tool.
10012/131 FIG. 8 is a side partial sectional view of an alternate embodiment of a temperature probe for use with a flowmeter in accordance with the present invention.
DETAILED DESCRIPTION OF INVENTION
10014/151 The method and system of the present disclosure will now be described more fully hereinafter with reference to the accompanying drawings in which embodiments are shown. The method and system of the present disclosure may be in many different forms and should not be construed as limited to the illustrated embodiments set forth herein; rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey its scope to those skilled in the art. Like numbers refer to like elements throughout.
100161 An example embodiment of a flowmeter assembly 20 is shown in a side perspective view in Figure 1. The flowmeter assembly 20 of Figure 1 is coupled with a tubular 22 in which a flow of fluid travels axially through the tubular 22. Included with the flowmeter assembly 20 is an electromagnetic source 24 that in the schematic example of Figure 1 circumscribes the outer periphery of the tubular 22. However, other examples exist wherein the electromagnetic source 24 projects along only a portion of the tubular 22 outer circumference.
Further illustrated in the example embodiment of Figure 1 is an aperture 25 provided through the wall of the tubular 22, and in a segment of the region where the tubular 22 is circumscribed by the electromagnetic source 24. An electromagnetic wave 26 is illustrated being directed into the fluid flow in the tubular 22 from the electromagnetic source 24. In an example embodiment, an optional window 27 may be set in the aperture 25, wherein the window 27 is designed to allow passage of electromagnetic waves that are within a designated range, such as the near infrared range or microwave range. The flowmeter assembly 20 of Figure 1 also includes a temperature probe 28 depicted set within the tubular 22. In the embodiment of Figure 1, the temperature probe 28 is at a location downstream of where the electromagnetic source 24 is located and at a distance X
from the point where the electromagnetic waves 26 enter the tubular 22. Lines 30, 31 are connected respectively to the probe 28 and electromagnetic source 24 on one end and that connect to a monitor 32 on the other end. The monitor 32 may be at a location remote from the electromagnetic source 24.
[0017] Figure 2 is a side partial sectional view of an alternate embodiment of the flowmeter assembly 20A wherein the tubular 22A is a modular section coaxially set in production tubing 33. The production tubing 33 is disposed within a wellbore 34 and is for flowing fluid extracted from a formation 36 up the wellbore 34 and to a wellhead assembly 38 set on an upper end of the wellbore 34. The tubular 22A of Figure 2 can be formed from material that can be penetrated by an electromagnetic wave 26 of the chosen wavelengths. Examples of material for the tubular 22A of Figure 2 include pure near-infrared-transparent materials such as perfluorocyclobutyl copolymers for near infrared or microwaves. For microwaves, material for the tubular 22A can be composites, either molded or wound, of epoxy, Kevlar0, glass, aramid, a polymer matrix, an epoxy resin, and combinations thereof Also in the example of Figure 2, the monitor 32 is set on surface above the opening of the wellbore 34 so that flow through the flowmeter assembly 20 can be remotely measured and recorded.
[0018] Figure 3 illustrates a side sectional view of an example of operation of the flowmeter assembly 20. In the example of Figure 3, fluid flow within the tubular 22 includes a first fluid 40 and second fluid 42. In an example embodiment, the first fluid 40 can be a hydrocarbon extracted from a subterranean formation, such as oil, and the second fluid 42 comprises water produced along with the hydrocarbon. As provided in Figure 1, and represented by the dashed line traversing the tubular 22 of Figure 3, a source line Ls illustrates the location in the tubular 22 where electromagnetic waves 261 are directed into the tubular 22. In the example of Figure 3, the electromagnetic waves 261 are designed to be absorbed by the first fluid 40 and thereby heat the fluid downstream of line L. To illustrate the heated effect, first fluid 40A is shown in a shaded view and downstream of line L. The electromagnetic waves 261 are chosen because their wavelength is absorbed by a particular fluid to heat that fluid, which in the example of Figure 3 is the first fluid 40. As such, the second fluid 42, does not absorb the particular electromagnetic waves 261, is not heated by the electromagnetic waves 261, and thereby stays at substantially the same temperature downstream of line Ls as it was upstream of line L.
[0019] Referring now to Figure 4, the heated first fluid 40A flows downstream of line Ls and proximate to the probe 28. The temperature of the stream downstream of line Ls changes in response to the heated first fluid 40A, the stream temperature change can be detected by monitoring stream temperature with the probe 28. Thus, in one example, the time between when the electromagnetic waves 261 are directed into the flowstream along line Ls and when the temperature difference in the fluid stream is detected by the temperature probe 28 is measured.
The velocity of the heated first fluid 40A can be estimated by dividing the measured time by the known distance X, which is the distance traveled by the heated first fluid 40A
after being heated and then being detected.
[0020] Similarly, as shown in Figure 5, velocity of the second fluid 42 can be estimated by directing an electromagnetic wave 262 into the fluid flow to form a heated second fluid 42A, then calculating the velocity of the second fluid by dividing the traveled time by the traveled distance as is described above in relation to Figure 4. The amplitude of the temperature response can be correlated to the volume fraction of that constituent in the flow stream. The flow quantity of that constituent can be estimated as the product of the flow velocity, cross-sectional area of the tubular, and volume fraction of that constituent. The flow quantity can be in terms of a volumetric flow rate or a mass flow rate.
[0021] In an alternate example provided in Figure 6, a pulse of electromagnetic waves 261 heats a plug of heated first fluid 40A in the flow shown flowing within the tubular 22 and across the probe 28. A series of pulses of electromagnetic waves 261, accompanied by continuously monitoring the temperature difference in the temperature probe 28, can provide a continuous real-time measurement of flow within the tubular 22. To avoid aliasing, the pulses can be separated in time by more than the fluid travel time between heating and detection. Optionally, a second probe 44 may be included within the tubular 22, wherein one of the probes 28, 44 is coated with an oil wet or water wet substance so that either only water or oil is sensed by the particular probe. In an example embodiment having both the oil wet and water wet probes, electromagnetic waves may be directed into the tubular for heating both water and oil simultaneously that may then be detected by the corresponding water or oil wet probe downstream in the fluid flow.
[0022] Referring now to Figure 7, a side partial sectional view is shown of an example where the flowmeter assembly 20A is disposed within an elongated downhole tool or sonde 46. In this example, the sonde 46 is inserted within production tubing 22 and into a fluid flow as shown by the arrows. An entrance (not shown) formed through a housing of sonde 46 enables the fluid flow to enter into the sonde 46 and make its way through the flowmeter assembly 20A. A
conveyance means 48, which can be a wireline, slick line, or coiled tubing, can be used to deploy the sonde 46 and flowmeter assembly 20A within the tubing 22. Communication from the flowmeter assembly 20A can be provided to surface through the conveyance means 48 and up into the wellhead assembly 38. The conveyance means 48 couples with a wire 50 inside the wellhead assembly 38 that then extends from the wellhead assembly 38 into the monitor 32 for relaying signals to and from the flowmeter assembly 20A and also enables control signals to be directed back into the wellbore 34 from the surface.
[0023] For contact temperature measurement, an alternate embodiment of a probe 28A is illustrated in Figure 8 that includes an array 52 of probes. The array 52 of Figure 8 includes thermocouples 54 suspended in the flow stream disposed strategically throughout the cross section of the tubular 22. Providing multiple thermocouples 54 as shown allows measuring a temperature distribution throughout the cross sectional area of the tubular 22. A matrix 56 of thin elongate members provides a mounting surface for the thermocouples 54.
Leads 58 between the thermocouples 54 and line 30A provide discrete communication to individual thermocouples 54 so the location in the tubular 22 where a signal is recorded can be correlated with the value of the signal. To improve thermal contact with the corresponding phase, selective thermocouples 54, such as every other thermocouple 54, could be coated with either an oil wet or water wet coating. Alternatively, probe 28 could be a non-contact sensor such as a pyroelectric detector.
[0024] In one example, the electromagnetic wave(s) is made up of an infrared wave and having a wave length of about 1,450 nanometers. Optionally, the wave length of the electromagnetic wave can be about 1,930 nanometers. When in this range, the electromagnetic wave is useful for , heating water within the fluid stream. In situations where it is desired to heat oil within the stream, an infrared wave having a wave length of about 1,740 nanometers can be used.
Optionally, microwaves can be used that in one example embodiment have frequencies that are about 15 MHz, and in another embodiment have a frequency of around 5 MHz. In this example, the heated fluid would be oil. For a microwave useful for heating water, the microwave has a frequency of about 18 GHz.
[0025] The scope of the claims should not be limited by the preferred embodiments set forth above, but should be given the broadest interpretation consistent with the description as a whole.
10012/131 FIG. 8 is a side partial sectional view of an alternate embodiment of a temperature probe for use with a flowmeter in accordance with the present invention.
DETAILED DESCRIPTION OF INVENTION
10014/151 The method and system of the present disclosure will now be described more fully hereinafter with reference to the accompanying drawings in which embodiments are shown. The method and system of the present disclosure may be in many different forms and should not be construed as limited to the illustrated embodiments set forth herein; rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey its scope to those skilled in the art. Like numbers refer to like elements throughout.
100161 An example embodiment of a flowmeter assembly 20 is shown in a side perspective view in Figure 1. The flowmeter assembly 20 of Figure 1 is coupled with a tubular 22 in which a flow of fluid travels axially through the tubular 22. Included with the flowmeter assembly 20 is an electromagnetic source 24 that in the schematic example of Figure 1 circumscribes the outer periphery of the tubular 22. However, other examples exist wherein the electromagnetic source 24 projects along only a portion of the tubular 22 outer circumference.
Further illustrated in the example embodiment of Figure 1 is an aperture 25 provided through the wall of the tubular 22, and in a segment of the region where the tubular 22 is circumscribed by the electromagnetic source 24. An electromagnetic wave 26 is illustrated being directed into the fluid flow in the tubular 22 from the electromagnetic source 24. In an example embodiment, an optional window 27 may be set in the aperture 25, wherein the window 27 is designed to allow passage of electromagnetic waves that are within a designated range, such as the near infrared range or microwave range. The flowmeter assembly 20 of Figure 1 also includes a temperature probe 28 depicted set within the tubular 22. In the embodiment of Figure 1, the temperature probe 28 is at a location downstream of where the electromagnetic source 24 is located and at a distance X
from the point where the electromagnetic waves 26 enter the tubular 22. Lines 30, 31 are connected respectively to the probe 28 and electromagnetic source 24 on one end and that connect to a monitor 32 on the other end. The monitor 32 may be at a location remote from the electromagnetic source 24.
[0017] Figure 2 is a side partial sectional view of an alternate embodiment of the flowmeter assembly 20A wherein the tubular 22A is a modular section coaxially set in production tubing 33. The production tubing 33 is disposed within a wellbore 34 and is for flowing fluid extracted from a formation 36 up the wellbore 34 and to a wellhead assembly 38 set on an upper end of the wellbore 34. The tubular 22A of Figure 2 can be formed from material that can be penetrated by an electromagnetic wave 26 of the chosen wavelengths. Examples of material for the tubular 22A of Figure 2 include pure near-infrared-transparent materials such as perfluorocyclobutyl copolymers for near infrared or microwaves. For microwaves, material for the tubular 22A can be composites, either molded or wound, of epoxy, Kevlar0, glass, aramid, a polymer matrix, an epoxy resin, and combinations thereof Also in the example of Figure 2, the monitor 32 is set on surface above the opening of the wellbore 34 so that flow through the flowmeter assembly 20 can be remotely measured and recorded.
[0018] Figure 3 illustrates a side sectional view of an example of operation of the flowmeter assembly 20. In the example of Figure 3, fluid flow within the tubular 22 includes a first fluid 40 and second fluid 42. In an example embodiment, the first fluid 40 can be a hydrocarbon extracted from a subterranean formation, such as oil, and the second fluid 42 comprises water produced along with the hydrocarbon. As provided in Figure 1, and represented by the dashed line traversing the tubular 22 of Figure 3, a source line Ls illustrates the location in the tubular 22 where electromagnetic waves 261 are directed into the tubular 22. In the example of Figure 3, the electromagnetic waves 261 are designed to be absorbed by the first fluid 40 and thereby heat the fluid downstream of line L. To illustrate the heated effect, first fluid 40A is shown in a shaded view and downstream of line L. The electromagnetic waves 261 are chosen because their wavelength is absorbed by a particular fluid to heat that fluid, which in the example of Figure 3 is the first fluid 40. As such, the second fluid 42, does not absorb the particular electromagnetic waves 261, is not heated by the electromagnetic waves 261, and thereby stays at substantially the same temperature downstream of line Ls as it was upstream of line L.
[0019] Referring now to Figure 4, the heated first fluid 40A flows downstream of line Ls and proximate to the probe 28. The temperature of the stream downstream of line Ls changes in response to the heated first fluid 40A, the stream temperature change can be detected by monitoring stream temperature with the probe 28. Thus, in one example, the time between when the electromagnetic waves 261 are directed into the flowstream along line Ls and when the temperature difference in the fluid stream is detected by the temperature probe 28 is measured.
The velocity of the heated first fluid 40A can be estimated by dividing the measured time by the known distance X, which is the distance traveled by the heated first fluid 40A
after being heated and then being detected.
[0020] Similarly, as shown in Figure 5, velocity of the second fluid 42 can be estimated by directing an electromagnetic wave 262 into the fluid flow to form a heated second fluid 42A, then calculating the velocity of the second fluid by dividing the traveled time by the traveled distance as is described above in relation to Figure 4. The amplitude of the temperature response can be correlated to the volume fraction of that constituent in the flow stream. The flow quantity of that constituent can be estimated as the product of the flow velocity, cross-sectional area of the tubular, and volume fraction of that constituent. The flow quantity can be in terms of a volumetric flow rate or a mass flow rate.
[0021] In an alternate example provided in Figure 6, a pulse of electromagnetic waves 261 heats a plug of heated first fluid 40A in the flow shown flowing within the tubular 22 and across the probe 28. A series of pulses of electromagnetic waves 261, accompanied by continuously monitoring the temperature difference in the temperature probe 28, can provide a continuous real-time measurement of flow within the tubular 22. To avoid aliasing, the pulses can be separated in time by more than the fluid travel time between heating and detection. Optionally, a second probe 44 may be included within the tubular 22, wherein one of the probes 28, 44 is coated with an oil wet or water wet substance so that either only water or oil is sensed by the particular probe. In an example embodiment having both the oil wet and water wet probes, electromagnetic waves may be directed into the tubular for heating both water and oil simultaneously that may then be detected by the corresponding water or oil wet probe downstream in the fluid flow.
[0022] Referring now to Figure 7, a side partial sectional view is shown of an example where the flowmeter assembly 20A is disposed within an elongated downhole tool or sonde 46. In this example, the sonde 46 is inserted within production tubing 22 and into a fluid flow as shown by the arrows. An entrance (not shown) formed through a housing of sonde 46 enables the fluid flow to enter into the sonde 46 and make its way through the flowmeter assembly 20A. A
conveyance means 48, which can be a wireline, slick line, or coiled tubing, can be used to deploy the sonde 46 and flowmeter assembly 20A within the tubing 22. Communication from the flowmeter assembly 20A can be provided to surface through the conveyance means 48 and up into the wellhead assembly 38. The conveyance means 48 couples with a wire 50 inside the wellhead assembly 38 that then extends from the wellhead assembly 38 into the monitor 32 for relaying signals to and from the flowmeter assembly 20A and also enables control signals to be directed back into the wellbore 34 from the surface.
[0023] For contact temperature measurement, an alternate embodiment of a probe 28A is illustrated in Figure 8 that includes an array 52 of probes. The array 52 of Figure 8 includes thermocouples 54 suspended in the flow stream disposed strategically throughout the cross section of the tubular 22. Providing multiple thermocouples 54 as shown allows measuring a temperature distribution throughout the cross sectional area of the tubular 22. A matrix 56 of thin elongate members provides a mounting surface for the thermocouples 54.
Leads 58 between the thermocouples 54 and line 30A provide discrete communication to individual thermocouples 54 so the location in the tubular 22 where a signal is recorded can be correlated with the value of the signal. To improve thermal contact with the corresponding phase, selective thermocouples 54, such as every other thermocouple 54, could be coated with either an oil wet or water wet coating. Alternatively, probe 28 could be a non-contact sensor such as a pyroelectric detector.
[0024] In one example, the electromagnetic wave(s) is made up of an infrared wave and having a wave length of about 1,450 nanometers. Optionally, the wave length of the electromagnetic wave can be about 1,930 nanometers. When in this range, the electromagnetic wave is useful for , heating water within the fluid stream. In situations where it is desired to heat oil within the stream, an infrared wave having a wave length of about 1,740 nanometers can be used.
Optionally, microwaves can be used that in one example embodiment have frequencies that are about 15 MHz, and in another embodiment have a frequency of around 5 MHz. In this example, the heated fluid would be oil. For a microwave useful for heating water, the microwave has a frequency of about 18 GHz.
[0025] The scope of the claims should not be limited by the preferred embodiments set forth above, but should be given the broadest interpretation consistent with the description as a whole.
Claims (12)
1. A method of measuring flow of a component of an oil and gas wellbore fluid stream, the method comprising:
a. installing a flowmeter in a production tube of the wellbore, the flowmeter comprising a transmitter device capable of transmitting at least two electromagnetic waves with different frequencies and a temperature sensor;
b. selecting an electromagnetic wave having a predetermined wavelength that is absorbed by a component that is expected to be present in the fluid stream;
c. heating the component by irradiating with the transmitter device the fluid stream with the electromagnetic wave having the wavelength that is absorbed by the component expected to be present in the fluid stream;
d. sensing with the temperature sensor a temperature of the fluid stream downstream of where the fluid stream is being irradiated;
e. detecting when the temperature of the fluid stream downstream of where the fluid stream is being irradiated increases due to heating with the electromagnetic wave; and f. estimating a velocity of the component expected to be present in the flow based on a distance between where the fluid stream is being irradiated and where the temperature of the fluid stream is being sensed and a time of heating of step (c) and a time of detecting of step (e).
a. installing a flowmeter in a production tube of the wellbore, the flowmeter comprising a transmitter device capable of transmitting at least two electromagnetic waves with different frequencies and a temperature sensor;
b. selecting an electromagnetic wave having a predetermined wavelength that is absorbed by a component that is expected to be present in the fluid stream;
c. heating the component by irradiating with the transmitter device the fluid stream with the electromagnetic wave having the wavelength that is absorbed by the component expected to be present in the fluid stream;
d. sensing with the temperature sensor a temperature of the fluid stream downstream of where the fluid stream is being irradiated;
e. detecting when the temperature of the fluid stream downstream of where the fluid stream is being irradiated increases due to heating with the electromagnetic wave; and f. estimating a velocity of the component expected to be present in the flow based on a distance between where the fluid stream is being irradiated and where the temperature of the fluid stream is being sensed and a time of heating of step (c) and a time of detecting of step (e).
2. The method of claim 1, wherein the component comprises a first component and the fluid stream comprises a second component, the method further comprises heating the second component by irradiating the fluid stream with an electromagnetic wave having a wavelength that is absorbed by the second component, repeating steps (d) and (e), and estimating a velocity of the second component based on the distance between where the fluid stream is being irradiated and where the temperature of the fluid stream is being sensed and the time of heating and the time of detecting of step (e).
3. The method of claim 2, wherein the first component comprises hydrocarbon.
4. The method of claim 2, wherein the first component comprises water.
5. The method of claim 4, wherein the frequency of the electromagnetic wave is 18 GHz.
6. The method of any one of claims 1 to 5, wherein the step of sensing temperature comprises sensing temperature at a plurality of discrete locations throughout a cross section of the fluid stream.
7. The method of claim 4, wherein the second component comprises oil.
8 The method of claim 7, wherein the electromagnetic wave to heat the first component has a wavelength with a value selected from 1450 nanometers and 1930 nanometers.
9 The method of claim 1, wherein the electromagnetic wave comprises at least one of a microwave and an infrared wave.
10. The method of claim 9, wherein the component expected to be present in the fluid stream comprises oil.
11. The method claim 10, wherein the frequency of the microwave is a value selected from 5 MHz and 15 MHz.
12. The method of claim 7, wherein the temperature sensor comprises an oil wet temperature probe and a water wet temperature probe.
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US13/173,173 US8656770B2 (en) | 2011-06-30 | 2011-06-30 | Electromagnetically heated thermal flowmeter for wellbore fluids |
US13/173,173 | 2011-06-30 | ||
PCT/US2012/043065 WO2013003109A2 (en) | 2011-06-30 | 2012-06-19 | Electromagnetically heated thermal flowmeter for wellbore fluids |
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CA2839763C true CA2839763C (en) | 2017-04-04 |
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Publication number | Priority date | Publication date | Assignee | Title |
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US10288463B2 (en) | 2015-06-26 | 2019-05-14 | Baker Hughes, A Ge Company, Llc | Multiphase thermal flowmeter for stratified flow |
NO342159B1 (en) * | 2016-02-16 | 2018-04-09 | Wellstarter As | A method and system for real-time fluid flow monitoring in a wellbore |
US11767753B2 (en) * | 2018-12-04 | 2023-09-26 | ExxonMobil Technology and Engineering Company | Method for flow profiling using transient active-source heating or cooling and temperature profiling |
GB2580445A (en) * | 2019-05-28 | 2020-07-22 | Equinor Energy As | Flow rate determination |
US11473412B2 (en) | 2020-10-12 | 2022-10-18 | Baker Hughes Oilfield Operations Llc | Selective heating of fluid components with microwaves to change viscosity ratio in downhole fluid devices |
CN112362121B (en) * | 2020-11-11 | 2021-07-02 | 东北石油大学 | Horizontal well oil-water two-phase flow measuring method based on thermal method |
CN114737950B (en) * | 2022-03-23 | 2024-04-19 | 燕山大学 | Horizontal gas-liquid two-phase flow near-infrared multi-detection point multi-parameter logging instrument and control terminal |
Family Cites Families (20)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3304766A (en) * | 1964-01-17 | 1967-02-21 | Texaco Inc | Method for measuring two-phase fluid flow |
US4228815A (en) * | 1975-06-19 | 1980-10-21 | Bayer Aktiengesellschaft | Measurement and control of multicomponent liquid systems |
US4059987A (en) * | 1976-10-20 | 1977-11-29 | Texaco Inc. | Apparatus and method for measuring the water content of oil flowing in a pipe |
US4190768A (en) * | 1978-06-29 | 1980-02-26 | Texaco Inc. | Determining the water cut and water salinity in an oil-water flow stream by measuring the sulfur content of the produced oil |
US4458709A (en) * | 1980-03-27 | 1984-07-10 | Binks Manufacturing Company | Method and apparatus for measuring and controlling fluid flow rates |
US4644263A (en) * | 1984-12-13 | 1987-02-17 | Marathon Oil Company | Method and apparatus for measuring water in crude oil |
US4813270A (en) * | 1988-03-04 | 1989-03-21 | Atlantic Richfield Company | System for measuring multiphase fluid flow |
US4891969A (en) * | 1988-07-07 | 1990-01-09 | Wayland J Robert | Oil/water ratio measurement |
US4938079A (en) * | 1989-03-06 | 1990-07-03 | Ivac Corporation | Thermal transit time flow measurement system |
US5297425A (en) * | 1992-03-23 | 1994-03-29 | Tennessee Valley Authority | Electromagnetic borehole flowmeter system |
US5386718A (en) * | 1992-06-02 | 1995-02-07 | Marathon Oil Company | Method for fluid analysis |
GB9305088D0 (en) * | 1993-03-12 | 1993-04-28 | Wrc Plc | Improvements in and relating to measurement of fluid flow velocity |
US5461909A (en) | 1993-05-21 | 1995-10-31 | Halliburton Logging Services, Inc. | Oxygen activation method for quantitative water flow measurements within and behind well bore casing |
US6386050B1 (en) * | 1999-12-21 | 2002-05-14 | Agilent Technologies, Inc. | Non-invasive fluid flow sensing based on injected heat tracers and indirect temperature monitoring |
FI114339B (en) * | 2001-05-16 | 2004-09-30 | Vaisala Oyj | Method and apparatus for determining the water content of a liquid |
GB2399111B (en) | 2003-03-07 | 2005-10-05 | Schlumberger Holdings | Methods for detecting while drilling underbalanced the presence and depth of water produced from the formation and for measuring parameters related thereto |
DE10356443A1 (en) * | 2003-12-03 | 2005-07-07 | Digmesa Ag | Method and device for non-contact measuring of flow rates |
US6874361B1 (en) | 2004-01-08 | 2005-04-05 | Halliburton Energy Services, Inc. | Distributed flow properties wellbore measurement system |
US7748265B2 (en) | 2006-09-18 | 2010-07-06 | Schlumberger Technology Corporation | Obtaining and evaluating downhole samples with a coring tool |
IL205614A0 (en) * | 2009-05-08 | 2010-11-30 | Renalsense Ltd | Device and method for monitoring renal function |
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US8656770B2 (en) | 2014-02-25 |
CA2839763A1 (en) | 2013-01-03 |
US20130000398A1 (en) | 2013-01-03 |
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EP2726709A2 (en) | 2014-05-07 |
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